Using the generating function of the Bessel functions, sometimes designated as G(x,t):
$$
\large
e^{\frac{x}{2}[t-t^{-1}]}=\sum_{n=-\infty}^{\infty}J_n(x)t^n\\[3em]
\xrightarrow{x=0} 1 = \sum_{n=-\infty}^{\infty}J_n(0)t^n =
\begin{align}&J_0(0) + \\&J_1(0) t + J_2(0) t^2 + ...\\&J_{-1}(0)t^{-1} + J_{-2}(0)t^{-2}+ ...\end{align}\\
$$
now by equating coefficients we get:
$$
J_0(0)=1\; \wedge \;J_{n\ne 0}(0)=0\\
\rightarrow J_0(\infty)=0
$$
Using the generating function of the Bessel functions, sometimes designated as G(x,t): $$ \large e^{\frac{x}{2}[t-t^{-1}]}=\sum_{n=-\infty}^{\infty}J_n(x)t^n\\[3em] \xrightarrow{x=0} 1 = \sum_{n=-\infty}^{\infty}J_n(0)t^n = \begin{align}&J_0(0) + \\&J_1(0) t + J_2(0) t^2 + ...\\&J_{-1}(0)t^{-1} + J_{-2}(0)t^{-2}+ ...\end{align}\\ $$ now by equating coefficients we get: $$ J_0(0)=1\; \wedge \;J_{n\ne 0}(0)=0\\ \rightarrow J_0(\infty)=0 $$